{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:YQ7ZFTKYGC3MW3DZR2J7BQR5JX","short_pith_number":"pith:YQ7ZFTKY","schema_version":"1.0","canonical_sha256":"c43f92cd5830b6cb6c798e93f0c23d4dfbdb3d311b5e3c3d5823f82d7e9adb14","source":{"kind":"arxiv","id":"1410.5586","version":1},"attestation_state":"computed","paper":{"title":"Six-dimensional weak-strong simulations of head-on beam-beam compensation in RHIC","license":"http://creativecommons.org/licenses/by/3.0/","headline":"","cross_cats":[],"primary_cat":"physics.acc-ph","authors_text":"A. Pikin (Brookhaven), G. Robert-Demolaize (Brookhaven), N.P. Abreu (Brookhaven), W. Fischer (Brookhaven), X. Gu (Brookhaven), Y. Luo (Brookhaven)","submitted_at":"2014-10-21T09:22:01Z","abstract_excerpt":"To compensate the large beam-beam tune spread and beam-beam resonance driving terms in the polarized proton operation in the Relativistic Heavy Ion Collider (RHIC), we will introduce a low-energy DC electron beam into each ring to collide head-on with the opposing proton beam. The device to provide the electron beam is called an electron lens. In this article, using a 6-D weak-strong-beam-beam interaction simulation model, we investigate the effects of head-on beam-beam compensation with electron lenses on the proton beam dynamics in the RHIC 250 GeV polarized proton operation. This article is"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1410.5586","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/3.0/","primary_cat":"physics.acc-ph","submitted_at":"2014-10-21T09:22:01Z","cross_cats_sorted":[],"title_canon_sha256":"59c3b21f393dfa30e876879d7a5a7cdb18c1adcd00fa21c3feccda529d9b5067","abstract_canon_sha256":"d859d7f3b3e83c78cbd5147b0747d6f6b93a3f3f1c862065286b8fb4bfc5478a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:39:39.509500Z","signature_b64":"+5MvJtQpPl4tk9yxlW9t7z5AFbQ1WpKBdV4Luzb8WpXpa3u77H8S6sni69zVTVciDdhNwCDOnswiv9T8IhKzAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c43f92cd5830b6cb6c798e93f0c23d4dfbdb3d311b5e3c3d5823f82d7e9adb14","last_reissued_at":"2026-05-18T02:39:39.509088Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:39:39.509088Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Six-dimensional weak-strong simulations of head-on beam-beam compensation in RHIC","license":"http://creativecommons.org/licenses/by/3.0/","headline":"","cross_cats":[],"primary_cat":"physics.acc-ph","authors_text":"A. Pikin (Brookhaven), G. Robert-Demolaize (Brookhaven), N.P. Abreu (Brookhaven), W. Fischer (Brookhaven), X. Gu (Brookhaven), Y. Luo (Brookhaven)","submitted_at":"2014-10-21T09:22:01Z","abstract_excerpt":"To compensate the large beam-beam tune spread and beam-beam resonance driving terms in the polarized proton operation in the Relativistic Heavy Ion Collider (RHIC), we will introduce a low-energy DC electron beam into each ring to collide head-on with the opposing proton beam. The device to provide the electron beam is called an electron lens. In this article, using a 6-D weak-strong-beam-beam interaction simulation model, we investigate the effects of head-on beam-beam compensation with electron lenses on the proton beam dynamics in the RHIC 250 GeV polarized proton operation. This article is"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1410.5586","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"1410.5586","created_at":"2026-05-18T02:39:39.509146+00:00"},{"alias_kind":"arxiv_version","alias_value":"1410.5586v1","created_at":"2026-05-18T02:39:39.509146+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1410.5586","created_at":"2026-05-18T02:39:39.509146+00:00"},{"alias_kind":"pith_short_12","alias_value":"YQ7ZFTKYGC3M","created_at":"2026-05-18T12:28:57.508820+00:00"},{"alias_kind":"pith_short_16","alias_value":"YQ7ZFTKYGC3MW3DZ","created_at":"2026-05-18T12:28:57.508820+00:00"},{"alias_kind":"pith_short_8","alias_value":"YQ7ZFTKY","created_at":"2026-05-18T12:28:57.508820+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/YQ7ZFTKYGC3MW3DZR2J7BQR5JX","json":"https://pith.science/pith/YQ7ZFTKYGC3MW3DZR2J7BQR5JX.json","graph_json":"https://pith.science/api/pith-number/YQ7ZFTKYGC3MW3DZR2J7BQR5JX/graph.json","events_json":"https://pith.science/api/pith-number/YQ7ZFTKYGC3MW3DZR2J7BQR5JX/events.json","paper":"https://pith.science/paper/YQ7ZFTKY"},"agent_actions":{"view_html":"https://pith.science/pith/YQ7ZFTKYGC3MW3DZR2J7BQR5JX","download_json":"https://pith.science/pith/YQ7ZFTKYGC3MW3DZR2J7BQR5JX.json","view_paper":"https://pith.science/paper/YQ7ZFTKY","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1410.5586&json=true","fetch_graph":"https://pith.science/api/pith-number/YQ7ZFTKYGC3MW3DZR2J7BQR5JX/graph.json","fetch_events":"https://pith.science/api/pith-number/YQ7ZFTKYGC3MW3DZR2J7BQR5JX/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/YQ7ZFTKYGC3MW3DZR2J7BQR5JX/action/timestamp_anchor","attest_storage":"https://pith.science/pith/YQ7ZFTKYGC3MW3DZR2J7BQR5JX/action/storage_attestation","attest_author":"https://pith.science/pith/YQ7ZFTKYGC3MW3DZR2J7BQR5JX/action/author_attestation","sign_citation":"https://pith.science/pith/YQ7ZFTKYGC3MW3DZR2J7BQR5JX/action/citation_signature","submit_replication":"https://pith.science/pith/YQ7ZFTKYGC3MW3DZR2J7BQR5JX/action/replication_record"}},"created_at":"2026-05-18T02:39:39.509146+00:00","updated_at":"2026-05-18T02:39:39.509146+00:00"}